University · Thermodynamics

Carnot Cycle Lab

Round 1/6Score: 0

Ideal heat engine

Amount of gas n
Hot reservoir Tₕ
Cold reservoir T꜀
Target work
2.0 L
2.00
50.0%
Net work per cycle
Heat supplied
Heat rejected
Actual efficiency

Live thermodynamic diagrams

Cycle path Enclosed work area Current state 1

Engine efficiency comparison

The Carnot engine sets the maximum theoretical efficiency for engines operating between the same hot and cold reservoir temperatures.

The physics

Ideal gas: pV = nRT, with R = 8.314 J/(mol K).

Carnot net work: W = nR(Tₕ − T꜀) ln(V₂/V₁).

Carnot efficiency: η꜀ = 1 − T꜀/Tₕ.

Carnot heat input: Qₕ = nRTₕ ln(V₂/V₁).

Otto-like efficiency: ηₒ = 1 − r^(1 − γ); γ = 1.4.

Otto-like constant-volume heating/cooling: Q = nCᵥΔT; Cᵥ = R/(γ − 1).

On a P–V diagram, net work equals the signed enclosed area ∮p dV. On a T–S diagram, reversible heat transfer equals ∫T dS.

Model: reversible ideal-gas cycles, fixed heat capacities, constant γ = 1.4. Volumes are in L on plots and converted to m³ for calculations. Pressures are in kPa. Carnot adiabats use TV^(γ−1) = constant. An Otto-like cycle has idealised isochoric heat transfer and adiabatic compression/expansion, with its minimum and maximum temperatures equal to T꜀ and Tₕ.